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1.
The formalism of projection Hamiltonians is applied to the N-component O(N)-invariant ϕ4 model in the Euclidean and p-adic spaces. We use two versions of the ε-expansion (with ε = 4 − d and with ε = α − 3d/2, where α is the renormalization group parameter) and evaluate the critical indices ν and η up to the second order of the perturbation theory. The results for the (4− d)-expansion then coincide with the known results obtained via the quantum-field renormalization-group methods. Our calculations give evidence that in dimension three, both expansions describe the same non-Gaussian fixed point of the renormalization group. __________ Translated from Teoreticheskaya i Matematicheskaya Fizika, Vol. 146, No. 3, pp. 365–384, March, 2006.  相似文献   

2.
A more intuitive sufficient condition is given for the concentration cancellation phenomena in 2- or 3-D incompressible fluid flows; that is, if the projection of concentration set of the weak-star defect measure associated with the approximate solution sequence onto space ℝπ x (n = 2, 3) is a set with Hausdorff dimension less than 1, then the weak-L 2 limit of the approximate solution sequence is a classical weak solution of Euler equation. Using this condition, an example is given to elucidate concentration-cancellation phenomena.  相似文献   

3.
We study in this paper solutions of the translation equation in rings of formal power series K[X] where K ∈R, C (so called one-parameter groups or flows), and even, more generally, homomorphisms Ф from an abelian group (G, +) into the group Г(K) of invertible power series in K[X]. This problem can equivalently be formulated as the question of constructing homomorphisms Ф from (G, +) into the differential group Г1∞ describing the chain rules of higher order of C∞ functions with fixed point 0. In this paper we present the general form of these homomorphisms Ф : G → Г(K) (or L1∞),Ф = (fn n≤1,forwhich f1 = l, f2 = ... = fp+l =0,fp+2 ≠ 0 for fixed, but arbitrary p ≤ 0 (see Theorem 5, Corollary 6 and Theorem 6). This representation uses a sequence (w n p )n≥p+2 of universal polynomials in fp+2 and a sequence of parameters, which determines the individual one-parameter group. Instead of (w n p )n≥p+2 we may also use another sequence (L n p )n≥p+2 of universal polynomials, and we describe the connection between these forms of the solutions.  相似文献   

4.
The time-dependent quantum Hamiltonians
describe a maser with N two-level atoms coupled to a single mode of a quantized field inside the maser cavity: here, ti, i=1,2,…,Na, are discrete times, Na is large (∼105), is the number operator in the Heisenberg-Weyl (HW) algebra, and ω0 is the cavity mode frequency. The N atoms form an (N+1)-dimensional representation of the su(2) Lie algebra, the single mode forming a representation of the HW algebra. We suppose that N atoms in the excited state enter the cavity at each ti and leave at ti+t int . With all damping and finite-temperature effects neglected, this model for N=1 describes the one-atom micromaser currently in operation with85Rb atoms making microwave transitions between two high Rydberg states. We show that is completely integrable in the quantum sense for any N-1,2,… and derive a second-order nonlinear ordinary differential equation (ODE) that determines the evolution of the inversion operator SZ(t) in the su(2) Lie algebra. For N=1 and under the nonlinear condition , this ODE linearizes to the operator form of the harmonic oscillator equation, which we solve. For N=1, the motion in the extended Hilbert space H can be a limit-cycle motion combining the motion of the atom under this nonlinear condition with the tending of the photon number n to n0 determined by (where r is an integer and g is the atom-field coupling constant). The motion is steady for each value of ti; at each ti, the atom-field state is |e>|n0>, where |e> is the excited state of the two-level atom and . Using a suitable loop algebra, we derive a Lax pair formulation of the operator equations of motion during the times t int for any N. For N=2 and N=3, the nonlinear operator equations linearize under appropriate additional nonlinear conditions; we obtain operator solutions for N=2 and N=3. We then give the N=2 masing solution. Having investigated the semiclassical limits of the nonlinear operator equations of motion, we conclude that “quantum chaos’ cannot be created in an N-atom micromaser for any value of N. One difficulty is the proper form of the semiclassical limits for the N-atom operator problems. Because these c-number semiclassical forms have an unstable singular point, “quantum chaos” might be created by driving the real quantum system with an additional external microwave field coupled to the maser cavity. 15 June–14 December 1997. Translated from Teoreticheskaya i Matematicheskaya Fizika, Vol. 122, No. 2, pp. 181–203, February, 2000.  相似文献   

5.
Under the assumption of (f, M n ,N 2n−1) being trivial, the classification of immersions homotopic tof: M n N 2n−1 is obtained in many cases. The triviality of (f, M n ,P 2n−1) is proved for anyM n andf. LetM, N be differentiable manifolds of dimensionn and2n−1 respectively. For a mapf: M → N, denote byI[M, N] f the set of regular homotopy classes of immersions homotopic tof. It has been proved in [1] that, whenn>1,I[M, N] f is nonempty for anyf. In this paper we will determine the setI[M, N] f in some cases. For example, ifN=P 2n−1 or more generally, the lens spacesS m 2n−1 =Z m /S 2n−1,M is any orientablen-manifold or nonorientable butn≡0, 1, 3 mod 4, then, for anyf, theI[M, N] f is determined completely. WhenN=R 2n−1, the setI[M, N] of regular homotopy classes of all immersions has been enumerated by James and Thomas in [2] and McClendon in [3] forn>3. Applying our results toN=R 2n−1 we obtain their results again, except for the casen≡2 mod 4 andM nonorientable. Whenn=3, McClendon's results cannot be used. Our results include the casesn=3,M orientable or not (for orientableM, I[M, R5] is known by Wu [4]).  相似文献   

6.
Let be a sequence of positive numbers and 1 ≤p < ∞. We consider the spacel P(β) of all power series such that . We give a necessary and sufficient condition for a polynomial to be cyclic inl P(β) and a point to be bounded point evaluation onl P(β).  相似文献   

7.
The absolute continuity of the spectrum for the periodic Dirac operator
, is proved given that A∈C(R n;R n)⊂H loc q(R n;R n), 2q>n−2, and also that the Fourier series of the vector potential A:R nR n is absolutely convergent. Here, are continuous matrix functions and for all anticommuting Hermitian matrices . Translated from Teoreticheskaya i Matematicheskaya Fizika, Vol. 124, No. 1, pp. 3–17, July, 2000.  相似文献   

8.
We study the asymptotics of the spectrum of the Maxwell operator M in a bounded Lipschitz domain W ì \mathbbR3 \Omega \subset {\mathbb{R}^3} under the condition of the perfect conductivity of the boundary ∂Ω. We obtain the following estimate for the remainder in the Weyl asymptotic expansion of the counting function N(λ,M) of positive eigenvalues of the Maxwell operator M:
N( l, M ) = \frac\textmeas W3p2l3( 1 + O( l - 2 / 5 ) ), N\left( {\lambda, M} \right) = \frac{{{\text{meas }}\Omega }}{{3{\pi^2}}}{\lambda^3}\left( {1 + O\left( {{\lambda^{{{{ - 2}} \left/ {5} \right.}}}} \right)} \right),  相似文献   

9.
If N ∈ ℕ, 0 < p ≤ 1, and(Xk) k=1 N are r.i.p-spaces, it is shown that there is C(= C(p, N)) > 0, such that for every ƒ ∈ ∩ k=1 N Xk, there exists with , for every 1 ≤ k ≤ N. Also, if ⊓ is a convex polygon in ℝ2, it is proved that the N-tuple (H(X1),…, H(Xn)) is K-closed with respect to (X1,…, XN) in the sense of Pisier. Everything follows from Theorem 2.1, which is a general analytic partition of unity type result.  相似文献   

10.
t , for t ≥ 0, be a strongly continuous Markovian semigroup acting on C(X), where X is a compact Hausdorf space, and let D denote the domain of its infinitesimal generator Z. Suppose D contains a (perhaps finite) family of functions f separating the points of X and satisfying Zf2 = 2fZf. If either (1) there exists δ > 0 such that (Tt f)2∈ D if 0 ≤ t ≤δ for each f in this family; or (1′) for some core D′ of Z, g ∈ D′ implies g2∈ D, then the underlying Markoff process on X is deterministic. That is, there exists a semiflow — a semigroup (under composition) of continuous functions φt from X into X — such that Ttf(x) = f(φt (x)). If the domain D should be an algebra then conditions (1) and (1′) hold trivially. Conversely, if we have a separating family satisfying Zf2 = 2fZf then each of these conditions implies that D is an algebra. It is an open question as to whether these conditions are redundant. If the functions φt are homeomorphisms from X onto X, then of course we have a Markovian group induced by a flow. This result is obtained by first providing general results about the null-space N of the (function-valued) positive semidefinite quadratic form defined by < f, g > = Z(fg) - fZg - gZf. The set N can be defined for any generator Z of a strongly continuous Markovian semigroup and is equivalently given by N = {f ∈ D| f2∈ D and Zf2 = 2fZf} = {f ∈ D| Tt(f2)-(Ttf)2 is o(t2) in C(X)}. In the general case N is an algebra closed under composition with any C1-function φ from the reals to the reals, and Z(φ[f]) = (Zf)φ′[f] if f ∈ N. This "chain rule" on N (on which Z must act as a derivation) is a special case of a theorem for C2-functions φ which holds more generally for all f in d, viz., Z(φ[f] = (Zf) φ′[f] + ? <f, f> φ″[f], Provided Z is a local operator and D is an algebra. In this case the form < f, g > itself enjoys the relation < φ[f], ψ[g] > = φ′ [f] ψ′[g] < f, g >, for C2functions φ and ψ. Some of the results and their proofs continue to hold when the setting is switched from the commutative C*-algebra C(X) to a general (noncommutative) C*-algebra A. In the norm continuous case we obtain a sharp characterization of Markovian semigroups that are groups: Let Tt = etz , defined for t ≥ 0, be a Markovian semigroup acting on a C*-algebra A that is norm continuous, i.e., ||Tt - I|| ⇒ 0 as t ⇒ 0 +. Assume Z(a2) = a(Za) + (Za) a for some (perhaps finite) set of self-adjoint elements a that generate a Jordan algebra dense among the self-adjoint elements of A. The etz , -∞ < t < ∞, is a group of Markovian operators.  相似文献   

11.
This paper analyses the properties of the family of self-similar solutions of the generalized Tricomi equation utt - t2k Du = 0 (2k ? \mathbbN)u_{{tt}} - t^{{2k}} \Delta u = 0\,(2k \in {{\mathbb{N}}}) in the domain \mathbbR + 1 + n{{\mathbb{R}}}_{ + }^{{1 + n}} by considering initial conditions on the functions and their derivatives, posed as the Cauchy problem with homogeneous initial data. For specific values of the power k ( = 1/2 or = 3/2) and n = 1 this problem has applications in the aerodynamics of airfoils operating in transonic flows of perfect or dense gases, respectively. An integral transformation is suggested and used to represent the solutions of the Cauchy problem with homogeneous initial functions in terms of fundamental solutions of the classical wave equation (the case k = 0). Then the Cauchy problem with homogeneous initial functions for the wave equation in \mathbbR1 + n{{\mathbb{R}}}^{{1 + n}} is solved. These results are used to derive estimates of the upper bound for solutions’ size and to obtain the asymptotics for self-similar solutions of the wave equation and of the Tricomi-type equation in the neighbourhood of their light cones.  相似文献   

12.
We investigate limiting behavior as γ tends to ∞ of the best polynomial approximations in the Sobolev-Laguerre space WN,2([0, ∞); e−x) and the Sobolev-Legendre space WN,2([−1, 1]) with respect to the Sobolev-Laguerre inner product
and with respect to the Sobolev-Legendre inner product
respectively, where a0 = 1, ak ≥0, 1 ≤kN −1, γ > 0, and N ≥1 is an integer.  相似文献   

13.
The following theorem is proved. Let N = h2n-1, where n ≥ 2, h is odd, 1 <-h < 2n, and suppose that v is a positive integer, v ≥ 3,α is a root of the equation $$(v^2 - 4,N) = 1,\left( {\frac{{v - 2}}{N}} \right) = 1,\left( {\frac{{v + 2}}{N}} \right) = - 1$$ . Then for N to be prime, it is necessary and sufficient that sn?2≡0(modN), where Sk+1=S k 2 ? 2 (k = 0, 1...), so=ah+ a?h. For given N, an algorithm is described for the construction of the smallest v satisfying the conditions of this theorem.  相似文献   

14.
Using the group <a,b|a3=b3=(ab)3=1>, we refute the conjecture dubbed in 1976 by V. Belyaev and N. Sesekin, which maintained that the growth function σ(n) of a finitely generated group satisfies the inequality σ(n)≤(σ(n−1)+σ(n+1))/2 for all sufficiently large n. Supported by the National Research Foundation of Switzerland, and by RFFR grant No. 96-01-00974. Translated fromAlgebra i Logika, Vol. 37, No. 6, pp. 621–626, November–December, 1998.  相似文献   

15.
In this paper, we study some nonlocal problems for the Kelvin-Voight equations (1) and the penalized Kelvin-Voight equations (2): the first and second initial boundary-value problems and the first and second time periodic boundary problems. We prove that these problems have global smooth solutions of the classW 1 (ℝ+;W 2 2+k (Ω)),k=1,2,...;Ω⊂ℝ3. Bibliography: 25 titles. Dedicated to N. N. Uraltseva on her jubilee Translated fromZapiski Nauchnykh Seminarov POMI, Vol. 221, 1995, pp. 185–207. Translated by N. A. Karazeeva.  相似文献   

16.
It is well known that the number of isolated singular points of a hypersurface of degree d in ℂPm does not exceed the Arnol’d number Am(d), which is defined in combinatorial terms. In the paper it is proved that if b m−1 ± (d) are the inertia indices of the intersection form of a nonsingular hypersurface of degree d in ℂPm, then the inequality Am(d)<min{b m−1 + (d), b m−1 (d)} holds if and only if (m−5)(d−2)≥18 and (m,d)≠(7,12). The table of the Arnol’d numbers for 3≤m≤14, 3≤d≤17 and for 3≤m≤14, d=18, 19 is given. Bibliography: 6 titles. Translated fromZapiski Nauchnykh Seminarov POMI, Vol. 231, 1995, pp. 180–190. Translated by O. A. Ivanov and N. Yu. Netsvetev.  相似文献   

17.
In this paper we establish a Serrin’s type regularity criterion on the gradient of pressure for weak solutions to the Navier–Stokes equations in It is proved that if the gradient of pressure belongs to Lα, γ with then the weak solution actually is regular and unique. Received: May 4, 2004  相似文献   

18.
We obtain a new upper bound for the sum Σ hH Δ k (N, h) when 1 ≤ HN, k ∈ ℕ, k ≥ 3, where Δ k (N, h) is the (expected) error term in the asymptotic formula for Σ N<n≤2N d k (n)d k (n + h), and d k (n) is the divisor function generated by ζ(s) k . When k = 3, the result improves, for HN 1/2, the bound given in a recent work of Baier, Browning, Marasingha and Zhao, who dealt with the case k = 3.  相似文献   

19.
Let p be an odd prime, c be an integer with (c, p) = 1, and let N be a positive integer with Np − 1. Denote by r(N, c; p) the number of integers a satisfying 1 ≤ aN and 2 ∤ a + ā, where ā is an integer with 1 ≤ āp − 1, c (mod p). It is well known that r(N, c; p) = 1/2N + O(p 1/2log2 p). The main purpose of this paper is to give an asymptotic formula for Σ c=1 p−1(r(N, c; p) − 1/2N)2.  相似文献   

20.
This paper which is a continuation of [2], is essentially expository in nature, although some new results are presented. LetK be a local field with finite residue class fieldK k. We first define (cf. Definition 2.4) the conductorf(E/K) of an arbitrary finite Galois extensionE/K in the sense of non-abelian local class field theory as wheren G is the break in the upper ramification filtration ofG = Gal(E/K) defined by . Next, we study the basic properties of the idealf(E/K) inO k in caseE/K is a metabelian extension utilizing Koch-de Shalit metabelian local class field theory (cf. [8]). After reviewing the Artin charactera G : G → ℂ ofG := Gal(E/K) and Artin representationsA g G → G →GL(V) corresponding toa G : G → ℂ, we prove that (Proposition 3.2 and Corollary 3.5) where Χgr : G → ℂ is the character associated to an irreducible representation ρ: G → GL(V) ofG (over ℂ). The first main result (Theorem 1.2) of the paper states that, if in particular,ρ : G → GL(V) is an irreducible representation ofG(over ℂ) with metabelian image, then where Gal(Eker(ρ)/Eker(ρ)•) is any maximal abelian normal subgroup of Gal(Eker(ρ)/K) containing Gal(Eker(ρ) /K)′, and the break nG/ker(ρ) in the upper ramification filtration of G/ker(ρ) can be computed and located by metabelian local class field theory. The proof utilizes Basmaji’s theory on the structure of irreducible faithful representations of finite metabelian groups (cf. [1]) and on metabelian local class field theory (cf. [8]). We then discuss the application of Theorem 1.2 on a problem posed by Weil on the construction of a ‘natural’A G ofG over ℂ (Problem 1.3). More precisely, we prove in Theorem 1.4 that ifE/K is a metabelian extension with Galois group G, then Kazim İlhan ikeda whereN runs over all normal subgroups of G, and for such anN, V n denotes the collection of all ∼-equivalence classes [ω]∼, where ‘∼’ denotes the equivalence relation on the set of all representations ω : (G/N) → ℂΧ satisfying the conditions Inert(ω) = {δ ∈ G/N : ℂδ} = ω =(G/N) and where δ runs over R((G/N)/(G/N)), a fixed given complete system of representatives of (G/N)/(G/N), by declaring that ω1 ∼ ω2 if and only if ω1 = ω 2,δ for some δ ∈ R((G/N)/(G/N)). Finally, we conclude our paper with certain remarks on Problem 1.1 and Problem 1.3.  相似文献   

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